PH403: Quantum Mechanics I Tutorial Sheet 2 This tutorial sheet deals with solutions of time-independent Schrödinger equation for simple potentials. 1. Consider the time-independent Schrödinger equation for a particle conned in one dimension, and exposed to a potential V (x). Show that across a nite discontinuity in the potential, the rst derivative of the wave function (x), i.e., 0(x), is continuous. 2. Consider a particle in a 1D box, i.e., a particle exposed to a potential V (x) which satises 1 for x < 0 and x > a V (x) = 0 otherwise. Solve the time-independent Schrödinger equation for this system to obtain its eigen- values and eigenfunctions. How will you generalize this solution if this potential well were in higher dimensions, i.e., 2D, and 3D. 3. Bound states in a nite potential well. Consider a particle of of mass m and energy E, subject to a potential dened by −V for x ≥ 0 and x ≤ a V (x) = 0 0 otherwise; where V0 > 0. Obtain the solutions of the time-independent Schrödinger equation for this system if 0 > E > −V0. 4. Consider a particle of mass m and energy E, incident from the left on a potential barrier dened by 0 for x < 0 V (x) = V0 x>0; where V0 > 0. Solve the Schrödinger equation for this system when (a) E < V0 , and (b) E > V0. For each case, calculate the reection coecient R, and transmission coecient T . Check any book on quantum mechanics to see the denitions of R and T . 5. Scattering from a nite 1D potential barrier. Consider a particle of mass m and energy E, incident from the left on a potential barrier dened by 0 for x < 0 and x > a V (x) = V0 otherwise; where V0 > 0. Solve the Schrödinger equation for this system when (a) E < V0 , and (b) E > V0. For each case, calculate the reection coecient R, and transmission coecient T . Note that as far as classical mechanics is concerned, no transmission is possible when E < V0. Nonzero value of T obtained quantum mechanically for this case is a manifestation of a phenomenon called tunneling. The fact that tunneling has been observed under a variety of situations experimentally, is yet another feather in the cap of quantum mechanics. 1 6. Bound state of particle in a delta-function potential. Consider a particle which is exposed to the 1D potential V (x) = −αδ(x); where α > 0 is a constant with suitable dimensions. (a) Integrate the time-independent Schrödinger equation between − and to obtain how the wave function and its rst derivative behave at the discontinuity at x = 0. (b) Assuming that the energy of the particle is E < 0, and the wave function is bound, obtain the possible values of E, and the corresponding wave functions. (c) Plot the wave functions and estimate their width ∆x. (d) What is the probability dP(p) that a measurement of the momentum of the particle in one of the normalized stationary states calculated above will give a result included between p and p + dp. For what value of p is this probability maximum? 7. Consider the potential of the previous problem. Assume that a particle with energy E > 0 is incident from the left on this potential. Calculate the coecients R and T for this system in terms of the dimensionless parameter , where 2 2. E=EL EL = −mα =2~ Study and analyze the variations of R and T with respect to E. 2.